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1 he NELF-B and NELF-D subunits at hundreds of interbands.
2 under visible light, which was attributed to interband absorption.
3  truly metallic nanotubes but show excitonic interband absorption.
4 were respectively ascribed to their LSPR and interband absorptions by Mie theory simulations and Drud
5 into a pattern of bands (afferent dense) and interband (afferent sparse) spaces that encompasses the
6 ed to study a new class of hamiltonians with interband and atom-molecule couplings.
7 ing which state filling induced bleaching of interband and exciton transitions curiously more than do
8 ganization of the chromosome by deleting the interband and fusing 3C7 with 3C6.
9 trolled, as a consequence of the intertwined interband and intraband electronic dynamics.
10                                              Interband and intraband electronic excitations in transi
11 it large ultrafast nonlinearities under both interband and intraband excitations.
12                            Using femtosecond interband and intraband spectroscopy, along with energy-
13 graphene conductivity are analyzed and their interband and intraband transition between modes are tho
14  localizes to Drosophila polytene chromosome interbands and phosphorylates histone H3 at interphase,
15         The Drosophila CHD1 localizes to the interbands and puffs of the polytene chromosomes, which
16 o less condensed, hypoacetylated euchromatic interbands and was absent from moderately condensed, hyp
17 D1 localizes to sites of extended chromatin (interbands) and regions associated with high transcripti
18 y parameters where findings indicate minimal interband Auger recombination.
19 rared absorption, an extensive bleach of the interband band-edge absorption, and a complete quenching
20                                          The interband cascade laser differs from any other class of
21                                          The interband cascade laser is consequently the most attract
22  simulations demonstrating that all previous interband cascade laser performance has suffered from a
23                   The instrument deploys two interband cascade lasers (ICL) with center wavelengths o
24 on spectroscopy (OF-CEAS) using mid-infrared interband cascade lasers (ICLs) is a sensitive technique
25 s the MsEph receptor is expressed by midline interband cells that are normally inhibitory to migratio
26 ures, we reveal two intermediate quasilinear interband contributions separated by a kink at 0.2 eV.
27 d, unconventional superconductors via strong interband Coulomb interaction, but is yet to be accessed
28 which the effective mass appears to diverge, interband coupling vanishes, and a local-moment state ap
29 arance of multiple plateaus indicates strong interband couplings involving multiple single-particle b
30 ch high power factors via a delayed onset of interband crossing.
31  Kerr effect, we detect and identify over 18 interband cyclotron resonances (CR) that are associated
32  small intraband Drude conductivity near the interband edge.
33 n unexpected behaviour that points to strong interband electron-electron scattering processes that co
34 iples and model calculations, we find strong interband electron-phonon coupling to play a crucial rol
35 xtraction by coupling photons generated from interband electronic transition to phonon polariton mode
36 encapsulated species also shifts the near-IR interband electronic transitions to lower energy by more
37 at into electricity and rejecting entropy by interband emission.
38 ogen-binding strength: Delta(dp) , the local interband energy separation between the lowest empty d-s
39                    This is attributed to the interband excitation of BiVO4, which is unfavourable for
40 e for low band gap semiconductors, for which interband excitations occur in wavelength regions that o
41 nnel than the bulk with no complication from interband excitations or need for reduced bulk doping.
42  3D topological insulator Bi2Se3 due to bulk interband excitations.
43 ntraband transition, a bleach of the visible interband exciton transitions, and a quench of the narro
44 lators, topological boundaries, and polytene interbands extends across the genome, and we therefore p
45 r between the layers due to layer-asymmetric interband hybridisation can generate a potential differe
46  located at the boundaries between bands and interbands in polytene chromosomes.
47                 When two bands have a strong interband interaction, the resulted electronic structure
48 on-coupling strength from the pi*-interlayer interband interaction.
49 ically compatible with the prominent role of interband interactions between symmetry-breaking Fermi p
50 A pol II in some but not all of the nonpuff, interband loci.
51 lectronic structures simultaneously suppress interband loss and boost the plasmonic response, ultimat
52  behavior remains elusive, primarily because interband losses arrest the propagation of infrared mode
53                                    We report interband magneto-optical spectra for single-walled carb
54 pidly along the bands (but not onto adjacent interband musculature) and then complete their different
55 s between them correspond with the bands and interbands of polytene chromosomes of Drosophila.
56 asm, and to several transcriptionally active interbands of polytene chromosomes.
57          With the spin-momentum locking, the interband optical pumping can renormalize the surface el
58 roperties is explained by the suppression of interband optical transitions and a small intraband Drud
59                                          The interband optical transitions cover a wide, technologica
60 arises from Coulomb repulsion due to virtual interband or excitonic processes.
61 iubov Fermi surfaces if spin-orbit coupling, interband pairing and time reversal symmetry breaking ar
62 o-dimensional superconductor is driven by an interband pairing interaction associated with nearly nes
63 axation, and radiative recombination through interband pathways and annihilation of defect-bound exci
64 otoactivation (internal photoemission versus interband photoexcitation followed by electron transfer)
65 e monolayer can be effectively raised by the interband photoexcitations in the SrTiO(3) substrate.
66 sual treatment, including both intraband and interband processes, considering the finite-temperature
67  and hole amplitude modes assisted by strong interband quantum entanglement. Such light-control of Hi
68                         We found evidence of interband recombination from photoexcited electron-hole
69 phasing, intraband relaxation, trapping, and interband recombination of free and trapped charge carri
70  fact that it localizes properly to polytene interband regions and that it contains both kinase domai
71  in which decompaction of boundary-insulator-interband regions drives the organization of interphase
72 s show that JIL-1 localizes to the gene-rich interband regions of larval polytene chromosomes and is
73 ophila localizes specifically to euchromatic interband regions of polytene chromosomes and is enriche
74 distributed filopodia onto both the band and interband regions of the midgut surface.
75 lements and the locations of mapped polytene interband regions.
76 gut, but the neurons strictly avoid adjacent interband regions.
77                                 However, the interband relaxation showed a strong time dispersion acr
78  convergence can be intrinsically negated by interband scattering depending on the manner in which ba
79 verge at a one k-point, which induces strong interband scattering of both the deformation-potential a
80 this advantage hinges on the assumption that interband scattering of carriers is weak or insignifican
81 i level, charge carriers can undergo intense interband scattering, yielding an energy filtering effec
82 inuous translational symmetry which leads to interband screening; so, dispersionless plasmons are a u
83                    fa(swb) is located in the interband separating polytene band 3C7, which contains N
84 ction segregates into a pattern of bands and interband spaces, and by P12 adult-like, afferent-dense
85 ally dependent correlation effects, enhanced interband spin fluctuations, or a Lifshitz-like transiti
86 pamin had the opposite effects on intra- and interband synchronization.
87  increased intraband synchrony and decreased interband synchrony, whereas apamin had the opposite eff
88 HPhP electroluminescence can arise from both interband transition and intraband Cherenkov radiation(8
89 tion splitting the Ru-H2 complex involves an interband transition in RuO2 which effectively diminishe
90  lattice vibrations coupled to an electronic interband transition naturally give rise to electron-ele
91 l relaxation pathway: Following an ultrafast interband transition, a void nanometer-sized bubble form
92 ement around 490 nm, which is ascribed to an interband transition.
93 m dots (QDs) emitting at 1.7 mum through the interband transition.
94 the energy and side-slope ratios between the interband-transition peaks at high energies in the exper
95                      This gate dependence of interband transitions adds a valuable dimension for opti
96 electronic effects, related to the nature of interband transitions and band edge localization under p
97 the combination of bulk charge carriers from interband transitions and surface charge carriers of the
98 troscopy, we find that they also have strong interband transitions and that their optical transitions
99  nanotubes is used to verify the energies of interband transitions and validate the spectral assignme
100                                 We show that interband transitions associated with the superlattice m
101         We show that the CPGE can arise from interband transitions at the metal contacts to silicon n
102 ound 0.4 electronvolts, which stems from the interband transitions between the nested subbands in lat
103 om temperature is observed, arising from the interband transitions between the subbands of 2D InAs na
104 ing contributions of the plasma dynamics and interband transitions beyond the approximations of the m
105 nce quantum, AQ = pialpha/nc for each set of interband transitions in a 2D semiconductor, where alpha
106 d based on existing models that include only interband transitions in ferromagnetic metals.
107 nocrystals (NCs) are characterized by strong interband transitions in the blue part of the spectral r
108  is sufficient to remove all vestiges of the interband transitions in the infrared spectrum.
109 tical conductivity above and below 0.2 eV to interband transitions near the double Weyl fermion and a
110  with the important influence of the X-point interband transitions on the intraband electron relaxati
111 ons, producing hotter electrons in gold, but interband transitions remain dominant.
112 llic band structure with a large bandgap for interband transitions responsible for semiconductor-meta
113 ave extended the accessible excitations from interband transitions to phonons.
114 strate how switching from intraband Ohmic to interband tunneling regime can raise detectors' responsi
115                                              Interband tunnelling of carriers through a forbidden ene
116 tor dependent and can be stabilized when the interband Weyl fermion scattering is dominant.

 
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